TY - JOUR
T1 - Lower bounds on Δms,d from constrained minimal flavour violation
AU - Blanke, Monika
AU - Buras, Andrzej J.
PY - 2007/5/1
Y1 - 2007/5/1
N2 - We demonstrate that in the class of models with Constrained Minimal Flavour Violation (CMFV), in which the CKM matrix is the only source of CP violation and B0q-0q mixings (q ≤ d,s) are described by a single operator (q)V-A(q)V-A, the lower bounds on the mass differences ΔMs,d are simply given by their Standard Model values (ΔMs,d)SM with two possible exceptions that we identify. Our proof involves all possible charged gauge boson, Goldstone boson and physical charged and neutral scalar exchanges and assumes that the masses of new charge +2/3 singlet heavy fermions Ti that mix with the top quark have all to be larger than mt, which is chosen by nature. Similarly, the additional charged gauge bosons have to satisfy Mi>MW, while no such bound needs to be set on the charged and neutral scalar masses. The two possible exceptions arise in the presence of U(1) neutral gauge bosons and Majorana fermions in box diagrams with flavour violating couplings. However in the case of the MSSM with CMFV and low tan β our bound is satisfied in spite of gluino and neutralino contributions.
AB - We demonstrate that in the class of models with Constrained Minimal Flavour Violation (CMFV), in which the CKM matrix is the only source of CP violation and B0q-0q mixings (q ≤ d,s) are described by a single operator (q)V-A(q)V-A, the lower bounds on the mass differences ΔMs,d are simply given by their Standard Model values (ΔMs,d)SM with two possible exceptions that we identify. Our proof involves all possible charged gauge boson, Goldstone boson and physical charged and neutral scalar exchanges and assumes that the masses of new charge +2/3 singlet heavy fermions Ti that mix with the top quark have all to be larger than mt, which is chosen by nature. Similarly, the additional charged gauge bosons have to satisfy Mi>MW, while no such bound needs to be set on the charged and neutral scalar masses. The two possible exceptions arise in the presence of U(1) neutral gauge bosons and Majorana fermions in box diagrams with flavour violating couplings. However in the case of the MSSM with CMFV and low tan β our bound is satisfied in spite of gluino and neutralino contributions.
KW - B-physics
KW - Beyond standard model
UR - http://www.scopus.com/inward/record.url?scp=34547564658&partnerID=8YFLogxK
U2 - 10.1088/1126-6708/2007/05/061
DO - 10.1088/1126-6708/2007/05/061
M3 - Article
AN - SCOPUS:34547564658
SN - 1126-6708
VL - 2007
JO - Journal of High Energy Physics
JF - Journal of High Energy Physics
IS - 5
M1 - 061
ER -